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and electrochemical properties of both
electron donor and acceptor play impor-
tant roles in controlling the morphology,
light harvesting properties, and photovol-
taic performance of the solar cells made
of those molecules. Although several
new high-performance donor materials
have emerged in the past few years, the
development of nonfullerene acceptors
(NFAs) is still in the infancy.
[4]
The most
successful and commonly used elec-
tron acceptors till date are fullerene and
its soluble derivative [6-6]-phenyl-C
61
/
C
71
-butyric acid methyl ester (PC
61
BM/
PC
71
BM).
[5]
However, the main drawbacks
associated with the fullerene based accep-
tors are their weak light absorption in the
visible range of the solar spectrum, wide
bandgap, and high synthesis cost.
[6,7]
In contrast, the NFAs can have several
advantages, such as tunable molecular
structure and energy levels, wide absorp-
tion range extended toward visible and
near IR region of solar spectrum, facile
synthesis, easy purifications, and low
cost. The most widely investigated struc-
tural templates for NFAs are perylenedi-
imide derivatives,
[4,8–10]
benzothiadiazole,
[11]
dicyanovinyl,
[12–16]
diketopyrrolopyrrole,
[7,16,17]
and rhodanines.
[18–20]
Another
promising NFA design is fluorine core flanked with the wings
of 3-ethylrhodanine, indandione, thiophene-2-carbonitrile
or, malononitrile. A high of PCE 7.16% was achieved from a
perylene bisimide (PBI) dimer based acceptor SdiPBI-S, devel-
oped by Sun et al.,
[21]
when blended with a wide bandgap
donor polymer PDBT-T1. Several electron acceptor moie-
ties, such as corannulene and truxenone having rotationally
symmetric polycyclic aromatic cores comprising 5th and 6th
membered ring have been developed for solution processable
organic photovoltaic (OPV) devices.
[22]
A phthalocyanine based
rotationally symmetric acceptor, labeled as Cl
6
-SubPc-Cl,
exhibited PCE of 6.86% with SubNc donor.
[23]
Calamitic
shaped small molecules have received immense attention
recently as an effective design strategy to develop a class of
high-performance NFAs. The acceptor 3,9-bis(2-methylene-
(3-(1,1-dicyanomethylene)-indanone))-5,5,11,11-tetrakis
(4-hexylphenyl)-dithieno[2,3-d:2′,3′-d′]-s-indaceno[1,2-b:5,6-b′]
dithiophene (ITIC) and donor poly[(2,6-(4,8-bis(5-(2-ethylhexyl)
thiophene-2-yl)-benzo[1,2-b:4,5-b ′ ]dithiophene))-alt-
(5,5-(1′,3′-di-2-thienyl-5′,7′-bis(2-ethylhexyl)benzo[1′,2′-c:4′,5′-c′]
dithiophene-4,8-dione))] (PBDB-T) based OPV device achieved
Molecular Engineering of Highly Efficient Small Molecule
Nonfullerene Acceptor for Organic Solar Cells
Suman, Vinay Gupta,* Anirban Bagui, and Surya Prakash Singh*
A new molecularly engineered nonfullerene acceptor,
2,2′-(5,5′-(9,9-didecyl-9H-fluorene-2,7-diyl)bis(benzo[c][1,2,5]thiadiazole-
7,4-diyl)bis(methanylylidene))bis(3-hexyl-1,4-oxothiazolidine-5,2-diylidene))
dimalononitrile (BAF-4CN), with fluorene as the core and arms of dicyano-
n-hexylrhodanine terminated benzothiadiazole is synthesized and used as
an electron acceptor in bulk heterojunction organic solar cells. BAF-4CN
shows a stronger and broader absorption with a high molar extinction
coefficient of 7.8 × 10
4
M
-1
cm
-1
at the peak position (498 nm). In the thin
film, the molecule shows a redshift around 17 nm. The photoluminescence
experiments confirm the excellent electron accepting nature of BAF-4CN
with a Stern–Volmer coefficient (K
sv
) of 1.1 × 10
5
M
-1
. From the electro-
chemical studies, the highest occupied molecular orbital and lowest unoc-
cupied molecular orbital energy levels of BAF-4CN are estimated to be
-5.71 and -3.55 eV, respectively, which is in good synchronization with
low bandgap polymer donors. Using BAF-4CN as an electron acceptor in a
poly[(5,6-difluoro-2,1,3-benzothiadiazol-4,7-diyl)-alt-(3,3″′-di(2-octyldodecyl)
2,2′;5′,2″;5″,2″′-quaterthiophen-5,5″′-diyl)] based bulk-heterojunction solar
cell, a maximum power conversion efficiency of 8.4% with short-circuit cur-
rent values of 15.52 mA cm
-2
, a fill factor of 70.7%, and external quantum
efficiency of about 84% covering a broad range of wavelength is achieved.
DOI: 10.1002/adfm.201603820
Suman, Dr. A. Bagui, Dr. S. P. Singh
Inorganic and Physical Chemistry Division
CSIR-Indian Institute of Chemical Technology (IICT)
Uppal Road, Tarnaka, Hyderabad 500007, India
E-mail: spsingh@iict.res.in
Suman, Dr. S. P. Singh
Academy of Scientific and Innovative
Research (AcSIR)
New Delhi 110 025, India
Dr. V. Gupta
Organic and Hybrid Solar Cell Group
CSIR-National Physical Laboratory
Dr. K. S. Krishnan Marg, New Delhi 110012, India
E-mail: drvinaygupta@netscape.net
1. Introduction
Molecular engineering of photoactive organic materials
for organic solar cell applications has emerged as a rapidly
growing research topic in recent years. Power conversion
efficiencies (PCEs) over 10% have been achieved from the
organic solar cells (OSCs) built with newly designed small-
molecule and polymeric materials.
[1–3]
The structural, optical,
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